CitThCavity Theory, Stopping -Power Ratios, Correction Factors. Alan E. Nahum PhD Physics Department Clatterbridge Centre for Oncology Bebington, Wirral CH63 4JY UK ((@
[email protected]) AAPM Summer School, CLINICAL DOSIMETRY FOR RADIOTHERAPY, 21-25 June 2009, Colorado College, Colorado Springs, USA 1 A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors. 313.1 INTRODUCTION 3.2 “LARGE” PHOTON DETECTORS 3.3 BRAGG-GRAY CAVITY THEORY 3.4 STOPPING-POWER RATIOS 3.5 THICK-WALLED ION CHAMBERS 363.6 CORRECTION OR PERTURBATION FACTORS FOR ION CHAMBERS 373.7 GENERAL CAVITY THEORY 3.8 PRACTICAL DETECTORS 3.9 SUMMARY 2 A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors. Accurate knowledgg(p)e of the (patient) dose in radiation therapy is crucial to clinical outcome For a given fraction size 100 TCP 80 (%) 60 Therapeutic Ratio NTCP 40 & NTCP 20 TCP 0 20 40 60Dpr 80 100 Dose (Gy) 3 A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors. Detectors almost never measure dose to medium directly. Therefore, the interpretation of detector reading requires dosimetry theory - “cavity theory” 4 A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors. D especially when converting med from calibration at Q to f Q 1 D measurement at Q2 5 det Q A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors. Also the “physics” of depth-dose curves: 6 A. E. Nahum: Cavity Theory, Stopping-Power Ratios, Correction Factors. Dose computation in a TPS Terma cfKf. Kerma 7 First we will remind ourselves of two key results which relate the particle fluence, , to energy deposition in the medium.